Method for forming identification marks on refractory material single crystal substrate, and refractory material single crystal substrate

ABSTRACT

An identification mark formation method for forming an identification mark on a refractory material single crystal substrate that is made of one selected from the group consisting of sapphire, gallium nitride, aluminum nitride, diamond, boron nitride, zinc oxide, gallium oxide, and titanium dioxide is disclosed. The method includes: (a) scanning a principal surface of the refractory material single crystal substrate with a laser beam at a first energy density such that a groove is formed in the principal surface of the refractory material single crystal substrate, thereby forming an identification mark in the principal surface of the refractory material single crystal substrate; and (b) scanning an inside of the groove of the refractory material single crystal substrate with a laser beam at a second energy density that is lower than the first energy density.

BACKGROUND

1. Technical Field

The present invention relates to a method for forming an identification mark on a refractory (high melting point) material single crystal substrate and particularly to a method for forming an identification mark on a refractory material single crystal substrate using a laser beam.

2. Description of the Related Art

In recent years, refractory materials, such as silicon carbide (SiC), gallium nitride (GaN), aluminum nitride (AlN), zinc oxide (ZnO), have been receiving attention as new materials for semiconductor devices or as new growth substrates for semiconductors. For example, the silicon carbide semiconductor has a larger dielectric breakdown electric field, a faster saturated drift velocity of electrons, and a greater thermal conductivity than those of the silicon semiconductor. Thus, research and development have been intensively carried out for realizing a power device which is capable of a large current operation at a high temperature and at a high speed with the use of a silicon carbide semiconductor as compared with conventional silicon devices. Among others, motors for use in electric motorcycles, electric vehicles, and hybrid vehicles are AC-driven or inverter-controlled, and therefore, development of efficient switching devices for such uses has been receiving attention. To realize such power devices, a silicon carbide single crystal substrate for epitaxial growth of a high-quality silicon carbide semiconductor layer is necessary.

Demands for blue laser diodes which are used as a light source for recording data at a high density and white diodes which are used as a light source in place of a fluorescent lamp or an incandescent bulb have been growing. Such light-emitting devices are manufactured using a gallium nitride semiconductor, and in some cases, a wide-bandgap compound semiconductor substrate such as a silicon carbide single crystal substrate is used as the substrate for formation of a high-quality gallium nitride semiconductor layer. Therefore, there is demand for a wide-bandgap compound semiconductor substrate which is used as a substrate for manufacture of a semiconductor device for which demand is expected to undergo a large growth in the future, such as a silicon carbide semiconductor device, a gallium nitride semiconductor device, etc.

To a semiconductor substrate which is used for manufacture of a semiconductor device, information for identification is provided as an identification mark for identifying semiconductor substrates and managing the process conditions of the manufacture process through which they have undergone for each of the semiconductor substrates. Usually, the identification mark has a size which is perceivable by a human eye. However, in other cases, the identification mark is imaged by a camera or the like and image-processed so as to be detected by a semiconductor manufacturing apparatus or the like.

In forming an identification mark on a semiconductor substrate, a laser beam is usually used. The semiconductor in a region irradiated with a laser beam is melted and evaporated, whereby a recessed portion is formed in the surface of the semiconductor substrate. The recessed portion constitutes an identification mark. According to the depth of this recessed portion, the method for forming an identification mark is generally divided into two types. Specifically, formation of an identification mark with a recessed portion depth of about 0.1 μm to 5 μm is referred to as “soft marking”, and formation of an identification mark with a recessed portion depth of about 5 μm to 100 μm is referred to as “hard marking”. Also, in some cases, the identification mark is constituted of a recessed portion which is in the form of an independent dot, and in other cases, the identification mark is constituted of one or more linear grooves.

The above-described refractory semiconductor is a new semiconductor material and has a higher melting point than other semiconductor materials which are widely employed, such as silicon, gallium arsenide, etc. Therefore, it is generally difficult to form a desirable identification mark on a refractory single crystal substrate under the conditions that are suitable for formation of an identification mark on a silicon substrate. Japanese Laid-Open Patent Publication No. 2006-43717 (hereinafter, referred to as Patent Document 1) discloses the technique of forming an identification mark which has an excellent visibility, which is realized by irradiating a silicon carbide single crystal substrate with pulsed laser light which has a predetermined pulse shape such that the silicon carbide is melted, whereby a slightly-recessed region is formed which contains a greater amount of carbon or silicon.

SUMMARY

According to the method of Patent Document 1, an identification mark which is constituted of a slightly-recessed dot is formed. Therefore, it is inferred that, according to the method of Patent Document 1, the identification mark which is constituted of the dot is formed by soft marking. Formation of the identification mark by soft marking is usually performed on a mirror-finished semiconductor substrate in many cases. However, since formation of the identification mark leads to formation of a bump in the substrate, there is a problem that the flatness of the substrate is marred.

Patent Document 1 discloses that a recessed portion in the form of a dot which constitutes an identification mark is formed by a region which contains a greater amount of carbon or silicon, whereby the perceivability which is attributed to reflected light and transmitted light is improved. However, there is a problem that an identification mark which is constituted of a dot is intrinsically inferior in visibility to an identification mark which is constituted of a line. Further, the recessed portion in the form of a dot which constitutes the identification mark has a small size, and therefore, laser dust, such as a solidified substance of silicon carbide melted by laser irradiation, abrasive grains, or other minute contaminants which can be produced in the middle of the semiconductor manufacturing process readily remain in the recessed portion in the form of a dot. Such contaminants remaining in the recessed portion can be a cause for contamination of the surface of the substrate when they are separated from the recessed portion, or a cause for formation of scars in the surface, in a substrate manufacturing process or a semiconductor device manufacturing process which would be performed later.

The present invention solves at least one of the above problems which arise in the prior art. One of the objects of the present invention is to provide a method for forming a highly-visible identification mark on a refractory material single crystal substrate.

An identification mark formation method of the present invention is a method for forming an identification mark on a refractory material single crystal substrate, the refractory material single crystal substrate being made of a single crystal which is formed by one selected from the group consisting of sapphire, gallium nitride, aluminum nitride, diamond, boron nitride, zinc oxide, gallium oxide, and titanium dioxide, the method comprising: (a) scanning a principal surface of the refractory material single crystal substrate with a laser beam at a first energy density such that a groove is formed in the principal surface of the refractory material single crystal substrate, thereby forming an identification mark which is constituted of one or more grooves in the principal surface of the refractory material single crystal substrate; and (b) scanning an inside of the groove formed in the principal surface of the refractory material single crystal substrate with a laser beam at a second energy density that is lower than the first energy density.

In a preferred embodiment, a width of the groove is not less than 50 μm, and a depth of the groove is not less than 10 μm.

In a preferred embodiment, the surface roughness Ra of an internal surface of the groove is not more than 1 μm.

In a preferred embodiment, the method further comprises (c) after step (b), performing mechanical polishing on the principal surface of the refractory material single crystal substrate.

In a preferred embodiment, after step (c), gas phase etching is performed on the principal surface of the refractory material single crystal substrate.

In a preferred embodiment, the surface roughness Ra of the principal surface of the refractory material single crystal substrate is not less than 0.1 nm and not more than 2.0 nm.

A refractory material single crystal substrate has an identification mark on a principal surface, the identification mark being constituted of one or more grooves, and the refractory material single crystal substrate being made of a single crystal which is formed by one selected from the group consisting of sapphire, gallium nitride, aluminum nitride, diamond, boron nitride, zinc oxide, gallium oxide, and titanium dioxide, wherein a width of the groove is not less than 50 μm and less than 0.5 mm, and a depth of the groove is not less than 10 μm, and a surface roughness Ra of an internal surface of the groove is not more than 1 μm.

In a preferred embodiment, a bottom surface of the groove is a solidified surface.

In a preferred embodiment, the bottom surface of the groove has a striped pattern.

According to the present invention, a refractory material single crystal substrate can be obtained that has an identification mark on which there is substantially no contaminant in a groove and which has excellent visibility.

Additional benefits and advantages of the disclosed embodiments will be apparent from the specification and Figures. The benefits and/or advantages may be individually provided by the various embodiments and features of the specification and drawings disclosure, and need not all be provided in order to obtain one or more of the same.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a schematic diagram showing a refractory material single crystal substrate in which an identification mark has been formed by methods of the first to third embodiments for forming an identification mark on a refractory material single crystal substrate.

FIG. 2 is a flowchart illustrating an embodiment of a method for forming an identification mark on a refractory material single crystal substrate according to the present invention.

FIG. 3A shows a scanning pattern of a laser beam in a rough laser step. FIG. 3B schematically shows a cross section of a groove formed in a principal surface of a refractory material single crystal substrate in the rough laser step.

FIG. 4A shows a scanning pattern of a laser beam in a finishing laser step. FIG. 4B schematically shows a cross section of a groove formed in a principal surface of a refractory material single crystal substrate in the finishing laser step.

FIGS. 5A and 5B are a schematic plan view and a schematic cross-sectional view of a groove formed in a mechanically-polished principal surface of a refractory material single crystal substrate.

FIG. 6 is a SEM image of a groove of an identification mark formed by the method of Example 1-3.

FIGS. 7A and 7B are surface profiles of a cross section perpendicular to, and a cross section parallel to, the extending direction of a groove which constitutes an identification mark which was formed by the method of Example 1-3.

FIG. 8 is a SEM image of a groove of an identification mark formed by the method of Comparative Example 1-1.

FIGS. 9A and 9B are surface profiles of a cross section perpendicular to, and a cross section parallel to, the extending direction of a groove which constitutes an identification mark which is formed by the method of Comparative Example 1-1.

FIG. 10 is an optical microscopic image of a groove of an identification mark formed by the method of Example 2-1.

FIGS. 11A and 11B are surface profiles of a cross section perpendicular to, and a cross section parallel to, the extending direction of a groove which constitutes an identification mark which was formed by the method of Example 2-1.

FIG. 12 is an optical microscopic image of a groove of an identification mark formed by the method of Example 2-2.

FIGS. 13A and 13B are surface profiles of a cross section perpendicular to, and a cross section parallel to, the extending direction of a groove which constitutes an identification mark which was formed by the method of Example 2-2.

FIG. 14 is an optical microscopic image of a groove of an identification mark formed by the method of Comparative Example 2-1.

DETAILED DESCRIPTION

In the specification of the present application, a refractory material single crystal substrate refers to a substrate (wafer) that is made of a semiconductor single crystal whose melting point is not less than 1800° C., or a single crystal substrate which is for growth of a semiconductor single crystal. Specifically, a refractory material single crystal substrate is made of a single crystal which is formed by one selected from the group consisting of silicon carbide, sapphire, gallium nitride, aluminum nitride, diamond, boron nitride, zinc oxide, gallium oxide, and titanium dioxide. The melting point, thermal conductivity, and hardness (Vickers hardness) of these materials are shown in Table 1.

TABLE 1 Sapphire SiC Al₂O₃ GaN AlN Diamond BN ZnO Ga₂O₃ TiO₂ Melting 2700 2040 2500 2200 3550 2700 1975 1725-1900 1870 Point (° C.) Thermal 400 42 130 340 2000 400 25 13 Conductivity (Wm⁻¹K⁻¹) Hardness 2500 2300 1250-1900 1700 9000 4500 400-600 750 1000 (Hv)

Each one of these refractory material single crystal substrates has a refractory. In general, this makes it difficult to form an identification mark using a laser beam. Some of these refractory material single crystal substrates whose hardness is greater than 1500 Hv have bad processability. Although gallium oxide and titanium dioxide have smaller hardnesses than 1500 Hv, gallium oxide and titanium dioxide also have bad processability because they have high cleavability.

On the other hand, there is demand for the technique of forming an identification mark with high visibility on such a refractory material single crystal substrate, for the purpose of manufacturing new semiconductor devices. In view of the above problems, the inventor of the present application conceived a novel method for forming an identification mark on a refractory material single crystal substrate and a novel refractory material single crystal substrate which has an identification mark.

First Embodiment

Hereinafter, the first embodiment of a method for forming an identification mark on a refractory material single crystal substrate according to the present invention is described with reference to the drawings. In the present embodiment, a silicon carbide single crystal substrate is used as the refractory material single crystal substrate. FIG. 1 schematically shows a silicon carbide single crystal substrate 10 in which an identification mark 14 is formed by a method for forming an identification mark on a silicon carbide single crystal substrate according to the first embodiment. The silicon carbide single crystal substrate 10 is made of silicon carbide single crystal. The polytype of the silicon carbide single crystal is not particularly limited. It may be any polytype of silicon carbide single crystal. The size and thickness of the silicon carbide single crystal substrate 10 are not particularly limited.

The silicon carbide single crystal substrate 10 has a pair of principal surfaces 10 a and 10 b. The identification mark 14 is formed in one principal surface 10 a. The plane orientation of the principal surfaces 10 a and 10 b is not particularly limited. The crystal axis of the silicon carbide single crystal and the normal lines of the principal surfaces 10 a and 10 b may be identical with each other (so-called “just substrate”). Alternatively, the normal lines of the principal surfaces 10 a and 10 b may form an angle which is greater than 0° with respect to the crystal axis of the silicon carbide single crystal (so-called “off substrate”). The principal surface 10 a that has the identification mark 14 is the rear surface, while the principal surface 10 b is the front surface on which a semiconductor device is to be formed.

The principal surface 10 b of the silicon carbide single crystal substrate 10 is preferably a mirror surface. Specifically, the surface roughness Ra of the principal surface 10 b is preferably not more than 2.0 nm. This is because a high-quality silicon carbide layer or gallium nitride layer is epitaxially grown on the principal surface 10 b for fabrication of a semiconductor device. The lower limit of the surface roughness Ra of the principal surface 10 b is not particularly limited. However, as the surface roughness Ra decreases, the processing of the principal surface 10 b requires a longer time, so that the productivity of the silicon carbide single crystal substrate 10 deteriorates. Thus, from the viewpoint of industrial mass productivity, the surface roughness Ra of the principal surface 10 b is preferably not less than 0.1 nm.

On the other hand, the principal surface 10 a has a surface roughness which is selected according to its use or specifications required of the silicon carbide single crystal substrate 10. Specifically, the principal surface 10 a may be a mirror surface or may be a surface finished by mechanical polishing. When the principal surface 10 a is a mirror surface, the surface roughness Ra of the principal surface 10 a is not more than 2.0 nm. When the principal surface 10 a is a surface finished by mechanical polishing, the surface roughness Ra of the principal surface 10 a is not less than 50 nm and not more than 1000 nm.

In the present embodiment, the identification mark 14 is formed in the vicinity of an orientation flat 12 of the silicon carbide single crystal substrate 10. However, the position of the identification mark 14 is not particularly limited. The identification mark 14 may be formed at any other position over the principal surface 10 a.

The identification mark 14 may be constituted of characters which are used in various languages, such as numerals, alphabets, Katakana characters, Hiragana characters, Kanji characters, etc., and symbols. The number of characters is not particularly limited. The identification mark 14 preferably has a size which is perceivable by a naked eye. For example, it is preferred that the size of a single character is 0.8 mm or 1.6 mm. The upper limit of the size of a single character of the identification mark 14 is not particularly limited. However, when the size of a single character is excessively large, formation of characters takes a long time. The groove width is preferably less than 0.5 mm.

As will be described in detail hereinbelow, the aforementioned alphanumeric characters which constitute the identification mark 14 are not an identification mark which is constituted of recessed portions in the form of dots but an identification mark which is constituted of linear grooves. To secure sufficient visibility for a naked eye, the depth of the groove is preferably not less than 10 μm, and the width of the groove is preferably not less than 50 μm. Note that the visibility depends on the difference in reflectance between the groove which constitutes the identification mark and its surrounding portion or on the substrate on which the identification mark is formed.

Hereinafter, a method for forming an identification mark on a silicon carbide single crystal substrate according to the present embodiment is described in detail with reference to FIG. 1 and the flowchart shown in FIG. 2.

First, a silicon carbide single crystal substrate 10 is provided (step S11). As described above, the size, thickness, and polytype of the silicon carbide single crystal substrate 10 and the directions of the normal lines of the principal surface 10 a and the principal surface 10 b are not particularly limited. The principal surface 10 b of the silicon carbide single crystal substrate 10 before formation of the identification mark 14 may have a surface roughness which is obtained after being finished by mechanical polishing or may be a mirror surface.

On the other hand, the principal surface 10 a preferably has a surface roughness which is obtained after being finished by mechanical polishing. This is because, when the surface roughness of the principal surface 10 a is generally equal to a surface roughness which is obtained after being finished by mechanical polishing, the laser beam for formation of the identification mark 14 is prevented from passing through the silicon carbide single crystal substrate 10 as compared with the case where the principal surface 10 a is a mirror surface, so that energy can be efficiently supplied to the principal surface 10 a of the silicon carbide single crystal substrate 10, and the groove of the identification mark 14 can be formed. Further, the principal surface 10 a of the silicon carbide single crystal substrate 10 may be directly irradiated with a laser beam such that the energy of the laser beam can be supplied to the principal surface 10 a, without providing an energy absorbing layer on the principal surface 10 a of the silicon carbide single crystal substrate 10 for absorbing the energy of the laser beam. Further, when the principal surface 10 a has a mirror surface before formation of the identification mark 14, the principal surface 10 a that is a mirror surface is mechanically polished after formation of the identification mark 14 as will be described later, and therefore, the previous mirror finishing step is of no use. In view of such circumstances, specifically, the surface roughness Ra of the principal surface 10 a is preferably not less than 50 nm and not more than 1000 nm. To sufficiently obtain the above-described effects, more preferably, the surface roughness Ra of the principal surface 10 a is not less than 100 nm and not more than 500 nm.

Then, the principal surface 10 a of the provided silicon carbide single crystal substrate 10 is scanned with a laser beam such that the identification mark 14 is formed in the principal surface 10 a. Formation of the identification mark is realized by forming the identification mark 14 which is constituted of one or more grooves by the rough laser process (step S12) and finishing the inside of the grooves by the finishing laser process (step S13). First, the rough laser process (step S12) is described.

As the laser light source which emits a laser beam for formation of the identification mark 14, a various types of laser light sources for use in laser marking may be used. Here, the laser light source may include not only a light-emitting light source which emits laser light but also an optical system which is used for adapting the beam diameter, a Q switch which is used for pulse driving of a laser beam, and a wavelength converter element which is used for adapting the wavelength of a laser beam. The laser light source which is used in the present embodiment is configured to emit a laser beam at a wavelength which is suitable to melting and evaporation of the silicon carbide single crystal. Specifically, the laser light source preferably emits a laser beam at a wavelength of not less than 532 nm and not more than 1064 nm. A laser light source which is configured to emit a laser beam at a wavelength shorter than 532 nm includes an expensive oscillator and is a large-size device. Therefore, particularly, the cost of forming an identification mark is likely to increase.

The beam diameter of the laser beam emitted from the laser light source depends on the size of the identification mark 14 which is to be formed and the power of the laser light source. For example, the laser light source emits a laser beam which has a beam diameter of, for example, not less than 5 μm and not more than 50 μm. The power of the laser light source is, for example, not less than 1.0 W and not more than 2.0 W. Using a laser light source whose power exceeds the upper limit is not preferred because there is a probability that damage, such as a slip, is caused in crystal.

The principal surface 10 a of the silicon carbide single crystal substrate 10 is scanned with a laser beam using a laser light source such that the identification mark 14 is formed in the principal surface 10 a. The principal surface 10 a is scanned at the first energy density such that a groove is formed in the principal surface 10 a of the silicon carbide single crystal substrate 10. FIG. 3A is a plan view schematically illustrating scanning with a laser beam. A pulsed laser beam is emitted from the laser light source to irradiate the principal surface 10 a with every single pulse of the laser beam which is represented by a beam spot 22 with the beam diameter R1 as shown in FIG. 3A. To irradiate the principal surface 10 a of the silicon carbide single crystal substrate 10 with the laser beam at a high energy density, the principal surface 10 a is preferably irradiated with the laser beam such that beam spots 22 each of which is formed by a single pulse successively overlap. As the overlapping area of the beam spots 22 increases, heat can be applied to the principal surface 10 a at a higher energy density. In this process, a groove 16 extending in a direction indicated by arrow 16 e is formed in the principal surface 10 a of the silicon carbide single crystal substrate 10.

In the case of the silicon carbide single crystal substrate 10, to form an identification mark 14 such that it is readily perceivable by a naked eye, the width of the groove 16 which constitutes the identification mark 14 is preferably not less than 50 μm, and the depth of the groove 16 is preferably not less than 20 μm. Usually, the beam diameter of the laser beam is about several micrometers, which is smaller than the preferred groove width. Therefore, it is preferred to form a groove which has a wider groove than the beam diameter of the laser beam by moving the laser beam for scanning in the extending direction of the groove 16 while the laser beam is also moved for scanning in a direction which is not parallel to the extending direction of the groove 16. Specifically, it is preferred to perform scanning according to a scanning pattern 24 which is zigzagged with respect to the extending direction of the groove 16. When scanning is performed with the laser beam with the kerf width W2, the groove 16 is formed which has the width W1 and which extends in a direction indicated by arrow 16 e.

By the laser beam irradiation, the silicon carbide single crystal is melted to a predetermined depth from the principal surface 10 a of the silicon carbide single crystal substrate 10, and the melted silicon carbide single crystal partially evaporates. Part of the melted silicon carbide which has not been evaporated then solidifies. As a result, the groove 16 which constitutes the identification mark 14 is formed in the principal surface 10 a of the silicon carbide single crystal substrate 10.

FIG. 3B shows a cross section of a groove 16 which is perpendicular to the extending direction of the groove which is indicated by arrow 16 e. The groove 16 includes a base surface 16 c and a pair of lateral surfaces 16 d between which the base surface 16 c extends. The base surface 16 c and the lateral surfaces 16 d form the internal surface 16 a of the groove 16. As shown in FIG. 3B, the internal surface 16 a of the groove 16 formed in the principal surface of the silicon carbide single crystal substrate 10 is formed by solidification of the melted silicon carbide single crystal. Also, minute solidified substances 18 of the solidified silicon carbide are attached onto the internal surface 16 a. On the principal surface 10 a extending outside the groove 16, there are also solidified substances or a bump 19 formed by solidification.

The solidified substances 18 produced inside the groove 16 and the solidified substances or bump 19 produced outside the groove 16 separate from the silicon carbide single crystal substrate 10 and attach to the principal surface 10 a and the principal surface 10 b of the silicon carbide single crystal substrate 10 as contaminants so that they can cause adverse effects, become the cause of scratches in the principal surface 10 a or the principal surface 10 b, or turn to dust to become the cause of contamination of other substrates or contamination inside the semiconductor device, in a subsequent step for fabrication of the silicon carbide single crystal substrate 10 or a manufacture step for manufacturing a semiconductor device using the completed silicon carbide single crystal substrate 10. For example, when an abrasive agent which is for use in the subsequent step that is for fabrication of the silicon carbide single crystal substrate 10 is brought into the groove 16, the abrasive agent is trapped by the internal surface 16 a because the surface roughness of the internal surface 16 a of the groove 16 is large, so that there is a probability that the abrasive agent cannot be removed from the groove 16 even by washing.

In the method for forming an identification mark on the silicon carbide single crystal substrate 10 according to the present embodiment, the finishing laser process (step S13) is performed, after the rough laser process, on the groove 16 which has been formed by the rough laser process in order to solve the above problems. By the finishing laser process, the solidified substances 18 and the bump 19 that have previously been described are again melted and evaporated such that the solidified substances 18 and the bump 19 are removed. Further, the internal surface 16 a is melted and solidified so as to have a smooth internal surface. The solidified substances 18, the bump 19, and the internal surface 16 a are formed by solidification of melted silicon carbide single crystal, so that they are amorphous or have low crystallinity. Further, in the rough laser process, carbon or silicon selectively evaporates, so that solidified substances 18, the bump 19, and the internal surface 16 a have a composition in which silicon or carbon is excessively contained or a composition in which silicon or carbon is bound to oxygen. These can be melted and evaporated even when the applied energy is not as large as the first energy density in the rough laser process.

Thus, by scanning the inside of the groove 16 which has been formed in the principal surface 10 a of the silicon carbide single crystal substrate 10 at the second energy density that is lower than the first energy density, the solidified substances 18 and the bump 19 can be removed, and also, the internal surface 16 a can be smoothed. Further, since the laser beam irradiation is performed at an energy density which is lower than the first energy density, a portion extending outside the groove 16 which is made of silicon carbide single crystal would not be newly melted or evaporated. That is, the laser beam irradiation is preferably performed at the second energy density such that the silicon carbide single crystal is not melted or evaporated. Thus, production of new solidified substances 18 or bump 19 by the finishing laser process is prevented. It is preferred that the ratio of the total energy of the finishing laser process to the total energy of the rough laser process is about not less than 10% and not more than 40%.

A pulsed laser beam is emitted from the laser light source to irradiate the inside of the groove 16 formed in the principal surface 10 a with every single pulse of the laser beam which is represented by a beam spot 22′ with the beam diameter R1 as shown in FIG. 4A. In FIG. 4A, the positions of the beam spot 22 in the rough laser process are shown by broken lines. As seen from FIG. 4A, the overlapping area of the beam spots 22′ is smaller than that of the beam spots 22 so that the second energy density is smaller than the first energy density. The other methods for decreasing the second energy density include decreasing the laser power and increasing the scanning speed.

Preferably as shown in FIG. 4A, the scanning direction of the laser beam in the step of the rough laser process and the scanning direction of the laser beam in the finishing laser process are different from each other. With this arrangement, the unevenness in the internal surface 16 a of the groove 16 which depends on the scanning direction of the laser beam in the step of the rough laser process is flattened in the finishing laser process, so that the inside of the groove 16 can be further smoothed. In the present embodiment, the inside of the groove 16 is scanned with the laser beam according to a scanning pattern 24′ which is parallel to the extending direction of the groove 16. As shown in FIG. 4A, it is preferred that a portion extending outside the groove 16 is also irradiated with the beam spots 22′ in order to remove the bump 19 which has been produced outside the groove 16 of the principal surface 10 a. With this arrangement, the wall surface of the groove 16 is also irradiated with the laser beam at a sufficient energy density, whereby the solidified substances 18 attached to the plane surface are removed, and the wall surface is smoothed. In other words, it is preferred that a region which is irradiated with the laser beam by the finishing laser process entirely includes a region which is irradiated with the laser beam in the step of the rough laser process and is also wider than a region which is irradiated with the laser beam in the rough laser process. Where a region which is irradiated with the laser beam in the rough laser process and a region which is irradiated with the laser beam in the finishing laser process are respectively referred to as the first region and the second region, the area of the second region is preferably 100% or more of the area of the first region. To remove the bump 19 which is produced outside the groove 16, the area of the second region is preferably 110% or more of the area of the first region.

As shown in FIG. 4B, by the finishing laser process, the solidified substances 18 which have been formed inside the groove 16 are removed, and the internal surface 16 b of the groove 16 is further smoothed. The bump 19 which has been produced outside the groove 16 of the principal surface 10 a is also removed. As a result of the finishing laser process, the surface roughness Ra is not more than 1 μm at the internal surface 16 b of the groove 16. Therefore, even when mechanical polishing, CMP (chemical mechanical polishing), or the like, is further performed on the principal surface 10 a in a subsequent step, the solidified substances 18 are prevented from separating from the groove and causing scratches in polishing of the principal surface 10 a. Also, since the internal surface 16 b of the groove 16 is smooth, the abrasive agent would not enter or reside in the groove 16.

The finishing laser process may be performed after the entirety of the identification mark 14 is formed by the rough laser process and the rough laser process is completed, or may be performed on parts of the identification mark 14 which have undergone the rough laser process one after another. In this case, the rough laser process and the finishing laser process are concurrently performed, and it is therefore preferred to provide a laser light source for the rough laser process and another laser light source for the finishing laser process. Where the pulse interval of the laser beam in the rough laser process is t and the interval between the rough laser process and the finishing laser process which are performed in an identical region of the identification mark 14 is T, T is sufficiently longer than t. That is, T>>t, so that part of the silicon carbide single crystal which is melted by the rough laser process is solidified and sufficiently cooled before the finishing laser process.

Formation of the identification mark 14 in the silicon carbide single crystal substrate 10 may be completed through the above-described processes. Alternatively, finishing of the identification mark 14 or finishing of the principal surface 10 a in which the identification mark 14 is provided may be performed. When mechanical polishing is performed on the principal surface 10 a of the silicon carbide single crystal substrate 10 in which the identification mark 14 has been formed such that the surface roughness of the principal surface 10 a is reduced, when there is a minute bump 19′ remaining outside the groove 16 of the principal surface 10 a and the bump 19′ is to be removed, or when the surface roughness of the internal surface 16 b of the groove 16 is further reduced, mechanical polishing is performed on the principal surface 10 a of the silicon carbide single crystal substrate 10 (step S14). Specifically, the principal surface 10 a of the silicon carbide single crystal substrate 10 is mechanically polished using a metal surface plate and an abrasive agent. In this process, the abrasive agent enters the inside of the groove 16 so that the internal surface 16 b of the groove 16 is also polished with the abrasive agent. As a result, as shown in FIGS. 5A and 5B, the silicon carbide single crystal substrate 10 is obtained in which the surface roughness of the internal surface 16 b′ is small and which has a principal surface 10 a′ with a reduced surface roughness. Further, the bump 19′ remaining outside the groove 16 also can be removed by this process.

To remove a damage layer which is formed over the surface of the principal surface 10 a of the silicon carbide single crystal substrate 10 due to the laser beam irradiation or solidification of melted silicon carbide, gas phase etching of the principal surface 10 a may be performed (step S15). Examples of the etching by the gas phase method which can be employed in the present embodiment include ion etching, sputter etching, reactive ion etching, plasma etching, reactive ion beam etching, and ion beam etching. Any other gas phase etching method may be employed.

The type of the gas used in the gas phase etching is not particularly limited. However, it is preferred to use a gas which contains fluorine, such as carbon tetrafluoride or sulfur hexafluoride or a gas which has reactivity with silicon carbide, such as hydrogen. Further, oxygen may be added in order to enhance oxidation. The conditions for the etching, such as the power to apply, depend on the apparatus used for the etching, for example. The etching rate preferably does not exceed 10 μm/h. If the etching rate exceeds 10 μm/h, the etching conditions would be excessively intense for the principal surface 10 a of the silicon carbide single crystal substrate 10 so that, probably, the principal surface 10 a is damaged by ion collision or the surface morphology of the principal surface 10 a after the etching deteriorates. Thus, this excessive etching rate is not preferred.

Since the thickness of the damage layer is small, the etching that is based on the gas phase method does not need to be performed for a long period of time. In the gas phase etching, the etching progresses generally uniformly so that the surface roughness of the principal surface 10 a scarcely varies. Thus, a principal surface can be obtained in which the surface roughness of the principal surface 10 a before the gas phase etching is generally maintained and from which the damage layer has been removed.

If the principal surface 10 b of the silicon carbide single crystal substrate 10 is a surface which is finished by mechanical polishing in formation of the above-described identification mark, mechanical polishing and mirror polishing may be performed on the principal surface 10 b after the formation of the identification mark.

By the method for forming an identification mark on a refractory material single crystal substrate according to the present embodiment, a silicon carbide single crystal substrate 10 with an identification mark 14 is obtained that is constituted of a groove 16 which has such a depth and a width that excellent visibility is achieved. Solidified substances 18 and the like are scarcely remaining in the groove 16 which constitutes the identification mark 14, and the internal surface 16 a has a surface roughness of not more than 1 μm. Therefore, even when mechanical polishing, CMP (chemical mechanical polishing), or the like, is further performed on the principal surface 10 a in a subsequent step, the solidified substances 18 are prevented from separating from the groove 16 and causing scratches in polishing of the principal surface 10 a. Also, since the internal surface 16 b of the groove 16 is smooth, the abrasive agent would not enter or reside in the groove 16. Thus, an excellent silicon carbide single crystal substrate 10 is obtained in which occurrence of various problems which are attributed to formation of the identification mark 14 is prevented in the process of fabricating the silicon carbide single crystal substrate 10 or in the process of manufacturing a semiconductor device.

Second Embodiment

Hereinafter, the second embodiment of a method for forming an identification mark on a refractory material single crystal substrate according to the present invention is described with reference to the drawings. In the present embodiment, a sapphire single crystal substrate is used as the refractory material single crystal substrate.

FIG. 1 schematically shows a sapphire single crystal substrate 10′ on which an identification mark 14 is formed by a method for forming an identification mark on a sapphire single crystal substrate according to the present embodiment. The sapphire single crystal substrate 10′ is made of sapphire single crystal.

The crystal orientation of the principal surface, and the like, of the sapphire single crystal substrate 10′ are not particularly limited as is the case with the first embodiment. The sapphire single crystal substrate 10′ may be a just substrate or may be an off substrate. As described in the first embodiment, the principal surface 10 b of the sapphire single crystal substrate 10′ is preferably a mirror surface. On the other hand, the principal surface 10 a in which an identification mark 14 is to be formed has a surface roughness which is selected according to its use or specifications required of the sapphire single crystal substrate 10′.

The identification mark formation method of the present embodiment for forming an identification mark on a sapphire single crystal substrate is the same as the identification mark formation method of the first embodiment for forming an identification mark on a silicon carbide single crystal substrate except that the laser irradiation conditions are different because of the different substrate materials. Specifically, a sapphire single crystal substrate 10′ is provided as previously described in the first embodiment with reference to FIG. 2 (step S11). The principal surface 10 a of the sapphire single crystal substrate 10′ is scanned with a laser beam to form an identification mark 14 in the principal surface 10 a. Formation of the identification mark is realized by forming the identification mark 14 which is constituted of one or more grooves by the rough laser process (step S12) and finishing the inside of the grooves by the finishing laser process (step S13). In the case of the sapphire single crystal substrate 10′, a preferred groove depth of an identification mark with excellent visibility is not less than 10 μm. A preferred groove width is 50 μm, which is the same as in the first embodiment. Thereafter, when necessary, mechanical polishing is performed on the principal surface 10 a of the sapphire single crystal substrate 10′ (step S14). Specifically, the principal surface 10 a of the sapphire single crystal substrate 10′ is mechanically polished using a metal surface plate and an abrasive agent. Also, when necessary, to remove a damage layer which is formed over the surface of the principal surface 10 a of the sapphire single crystal substrate 10′ due to the laser beam irradiation or solidification of melted sapphire, gas phase etching of the principal surface 10 a may be performed (step S15). As a result, the sapphire single crystal substrate 10′ on which an identification mark has been formed is obtained.

Now, the different aspects of the present embodiment from the first embodiment are mainly described. As described above, in the present embodiment, different laser irradiation conditions are employed from those of the first embodiment because of the different substrate material used. Specifically, in the present embodiment, it is preferred that the laser beam used for formation of the identification mark 14 has a shorter wavelength. Specifically, it is preferred that the wavelength of the laser beam is not less than 266 nm and not more than 532 nm.

It is preferred that the ratio of the total energy of the finishing laser process to the total energy of the rough laser process is about not less than 40% and not more than 95%. Since the sapphire single crystal itself is an oxide as is not the case with silicon carbide, the compositions of the solidified substances 18 and bump 19 generated by the rough laser process and the composition of the internal surface 16 a (FIG. 3B) are not largely different from that of the aluminum oxide that forms the sapphire single crystal substrate 10′. Therefore, the energy required for melting and evaporating the solidified substances 18 and bump 19 and the internal surface 16 a will not be much smaller than the energy of the laser beam in the rough laser process. Note that, however, the solidified substances 18 and bump 19 and the internal surface 16 a deviate from the composition of Al₂O₃ to have a composition of an oxide or to be in an amorphous or polycrystalline state. Therefore, the energy required for melting and evaporating the solidified substances 18 and bump 19 and the internal surface 16 a may be smaller than the energy required for formation of a groove in the rough laser process. Adjustment of the energy density in the rough laser process and the finishing laser process is carried out in the same way as that previously described in the first embodiment.

As seen from Table 1, the thermal conductivity of sapphire is smaller than the thermal conductivity of silicon carbide by about one order of magnitude. Therefore, in the case where a groove 16 is formed in the sapphire single crystal substrate 10′ by the rough laser process, heat is less likely to be transmitted to a region outside the groove which is not irradiated with the laser beam, and accordingly, melting and evaporation of sapphire abruptly occurs inside the groove 16, while increase in temperature of sapphire outside the groove 16 is prevented. As a result, the state of sapphire is largely different between the inside and outside of the groove 16, and a large stress occurs at the periphery of the groove 16 of the sapphire single crystal substrate 10′, so that cracks are likely to be generated.

To prevent generation of cracks, if the sum of the total energies supplied in the total process of the rough laser process and finishing laser process is constant, it is preferred that the difference in total energy between the rough laser process and the finishing laser process is smaller. Specifically, it is preferred that the ratio of the total energy for the finishing laser process to the total energy for the rough laser process is approximately not less than 80% and not more than 95%.

By the identification mark formation method of the present embodiment for forming an identification mark on a sapphire single crystal substrate, a sapphire single crystal substrate 10′ with an identification mark 14 is obtained that is constituted of a groove 16 which has such a depth and a width that excellent visibility is achieved. Solidified substances 18 and the like are scarcely remaining in the groove 16 which constitutes the identification mark 14, and the internal surface 16 a has a surface roughness of not more than 1 μm. Therefore, even when mechanical polishing, CMP (chemical mechanical polishing), or the like, is further performed on the principal surface 10 a in a subsequent step, the solidified substances 18 are prevented from separating from the groove 16 and causing scratches in polishing of the principal surface 10 a. Also, since the internal surface 16 b of the groove 16 is smooth, the abrasive agent would not enter or reside in the groove 16. Thus, an excellent sapphire single crystal substrate 10′ is obtained in which occurrence of various problems which are attributed to formation of the identification mark 14 is prevented in the process of fabricating the sapphire single crystal substrate 10′ or in the process of manufacturing a semiconductor device.

Third Embodiment

Hereinafter, the third embodiment of a method for forming an identification mark on a refractory material single crystal substrate according to the present invention is described with reference to the drawings. In the present embodiment, a gallium nitride single crystal substrate is used as the refractory material single crystal substrate.

FIG. 1 schematically shows a gallium nitride single crystal substrate 10″ on which an identification mark 14 is formed by a method for forming an identification mark on a gallium nitride single crystal substrate according to the present embodiment. The gallium nitride single crystal substrate 10″ is made of gallium nitride single crystal.

The polytype, the crystal orientation of the principal surface, and the like, of the gallium nitride single crystal substrate 10″ are not particularly limited as is the case with the first embodiment. The gallium nitride single crystal substrate 10″ may be a just substrate or may be an off substrate. As described in the first embodiment, the principal surface 10 b of the gallium nitride single crystal substrate 10″ is preferably a mirror surface. On the other hand, the principal surface 10 a in which an identification mark 14 is to be formed has a surface roughness which is selected according to its use or specifications required of the gallium nitride single crystal substrate 10″.

The identification mark formation method of the present embodiment for forming an identification mark on a gallium nitride single crystal substrate is the same as the identification mark formation method of the first embodiment for forming an identification mark on a silicon carbide single crystal substrate except that the substrate material is different. Specifically, a gallium nitride single crystal substrate 10″ is provided as previously described in the first embodiment with reference to FIG. 2 (step S11). The principal surface 10 a of the gallium nitride single crystal substrate 10″ is scanned with a laser beam to form an identification mark 14 in the principal surface 10 a. Formation of the identification mark is realized by forming the identification mark 14 which is constituted of one or more grooves by the rough laser process (step S12) and finishing the inside of the grooves by the finishing laser process (step S13). Thereafter, when necessary, mechanical polishing is performed on the principal surface 10 a of the gallium nitride single crystal substrate 10″ (step S14). Specifically, the principal surface 10 a of the gallium nitride single crystal substrate 10″ is mechanically polished using a metal surface plate and an abrasive agent. Also, when necessary, to remove a damage layer which is formed over the surface of the principal surface 10 a of the gallium nitride single crystal substrate 10″ due to the laser beam irradiation or solidification of melted gallium nitride, gas phase etching of the principal surface 10 a may be performed (step S15).

By the identification mark formation method of the present embodiment for forming an identification mark on a gallium nitride single crystal substrate, a gallium nitride single crystal substrate 10″ with an identification mark 14 is obtained that is constituted of a groove 16 which has such a depth and a width that excellent visibility is achieved.

Other Embodiments

As seen from Table 1, not only single crystal substrates of silicon carbide, sapphire, and gallium nitride but also single crystal substrates of aluminum nitride, diamond, boron nitride, zinc oxide, gallium oxide, and titanium dioxide have high melting points. By employing the identification mark formation methods described in the first to third embodiments for the single crystal substrates of these materials, an excellent refractory material single crystal substrate is obtained which has high visibility and in which occurrence of various problems that are attributed to formation of an identification mark 14 is prevented.

EXAMPLE 1

Hereinafter, an example of formation of an identification mark on a silicon carbide single crystal substrate with the use of a method for forming an identification mark on a silicon carbide single crystal substrate according to the first embodiment is described. A 4H silicon carbide single crystal substrate with a diameter of 3 inches was provided. The surface roughness Ra of the principal surface in which an identification mark was to be formed was 0.3 μm. The laser light source used was a Nd:YAG laser (wavelength: 1064 nm, power: 1.5 W) manufactured by ESI, Inc. This laser light source had a Q-switch and was used to perform the rough laser process and the finishing laser process under the conditions of Examples 1-1, 1-2, and 1-3 as shown in Table 2 such that an identification mark of nine characters was formed. In Comparative Example, only the rough laser process was performed for formation of an identification mark. In Table 2, the kerf width refers to W2 of FIG. 3. When the kerf width was 0, the principal surface of the substrate was scanned with a laser beam along a groove to be formed. For example, when the width of the groove was about three times the diameter of the laser beam, the principal surface was scanned with the laser beam such that spots in the left column shown in FIG. 3 were drawn, the principal surface was then scanned with the laser beam such that spots in the center column were drawn, and lastly, the principal surface was scanned with the laser beam such that spots in the right column were drawn. In Table 2, the energy density is a relative value which was determined with respect to the energy density of Comparative Example which was assumed as 100. In Examples 1-1, 1-2, and 1-3, the energy density of the finishing laser process was made smaller than the energy density of the rough laser process by nulling the kerf so as to shorten the scanning time per unit area. The total energy refers to a total energy which was supplied to the substrate by laser beam irradiation for marking a straight line of 1 mm in each of the rough laser process and the finishing laser process. The energy ratio refers to the ratio of the total energy of the finishing laser process to the total energy of the rough laser process.

After the formation of the identification mark by the laser, the principal surface in which the identification mark was formed was subjected to mechanical polishing with the use of a diamond slurry in which diamond particles with the average particle diameter of 5 μm were contained as the abrasive agent.

After the mechanical polishing, the inside of the groove constituting the identification mark was observed with an optical microscope to check whether there was an attached substance, such as a solidified substance, on the bottom surface and the lateral surfaces of the groove. Further, the depth and the width of the groove were measured using an optical length-measuring microscope. The measurement was performed at an arbitrary position in the groove, where the groove width on the substrate surface and the groove depth from the substrate surface were measured. The measurement was carried out at one arbitrary position in each of the grooves of three out of nine characters. Further, the surface roughness Ra of the bottom surface of the groove was measured using the optical interference type surface roughness measuring apparatus HD-2000 manufactured by Veeco Instruments Inc. The measurement was performed on a central portion at an arbitrary position in the groove, along the line direction (the longitudinal direction of the groove), in the length of about 0.2 mm. The measurement was carried out along one arbitrary line in each of the grooves of three out of nine characters. The results are shown in Table 3.

TABLE 2 Com- parative Example Example Example Exam- 1-1 1-2 1-3 ple 1-1 Rough Q rate (Hz) 7000 500 500 3000 Laser Power (%) 100 100 100 100 Process Speed (mm/s) 40 10 15 8 Kerf Width (mm) 0 0.08 0.08 0.15 Energy Density 70 75 72 100 Number of 3 1 1 1 Scanning Cycles Total Energy (W) 788 1200 1200 4200 Finish Q rate (Hz) 500 500 500 None Laser Power (%) 100 100 100 Process Speed (mm/s) 10 10 10 Kerf Width (mm) 0 0 0 Energy Density 10 10 10 Number of 3 3 5 Scanning Cycles (with offset) Total Energy (W) 225 225 375 Energy Ratio (%) 29 19 31

TABLE 3 Example Example Example Comparative Evaluated Items 1-1 1-2 1-3 Example 1-1 Attached Groove No No No Yes Substance Bottom Inside Wall No Yes No Yes Groove Surface Groove Before 45 50 50  60 Depth Polish (μm) Groove Before 45 100  110  150-170 Width Polish (μm) After 30 80 80 170 Polish Surface Roughness of 0.4-0.6 0.4-0.6 0.4-0.6 5.0-7.0 Groove Bottom Surface Ra (μm)

As seen from Table 3, no attached substance was found at the bottom surface of the groove in either of Examples 1-1, 1-2, and 1-3. In Examples 1-1 and 1-3, no attached substance was also found at the wall surface of the groove. On the other hand, in Comparative Example, attached substances were found at the bottom surface and the wall surface of the groove. This is probably because, in the methods of Examples 1-1, 1-2, and 1-3, solidified substances in the groove were removed by the finishing laser process. It was found from the results of Examples 1-1, 1-2, and 1-3 that attached substances can be entirely removed so long as the energy of the finishing laser process is approximately not less than 19% and not more than 31% of that of the rough laser process. It is understood that, when a margin of about 10% is considered, the energy ratio only needs to be approximately not less than 10% and not more than 40%.

In Example 1-2, the reason why there was an attached substance on the wall surface is probably that the laser beam of the finishing laser process failed to irradiate the wall surface inside the groove with a sufficient intensity. On the other hand, in Example 1-3, the finishing laser process was performed through five cycles, and in each scanning cycle, the position of the beam was offset by 0.02 mm. Therefore, it is inferred that the beam of the finishing laser process successfully uniformly irradiated the entire surface inside the groove.

In each of Examples 1-1, 1-2, and 1-3, the surface roughness Ra of the bottom surface of the groove of the formed identification mark was in the range of 0.4 μm to 0.6 μm. On the other hand, in Comparative Example, the surface roughness Ra of the bottom surface of the groove was in the range of 5.0 μm to 7.0 μm. It was found from this result that the surface roughness of the internal surface of the groove of the identification mark which was formed according to the methods of Examples 1-1, 1-2, and 1-3 was improved to about 1/10 of the surface roughness of the groove which was formed according to the conventional method. In Examples 1-1, 1-2, and 1-3 and Comparative Example, reduction of the surface roughness Ra by the mechanical polishing is estimated at about 50 nm to 100 nm, and therefore, the above-described difference in surface roughness Ra is not attributed to the mechanical polishing which is performed after the formation of the identification mark. In Examples 1-1, 1-2, and 1-3, it can be said that the surface roughness Ra of the bottom surface of the internal surface of the groove of the identification mark before the mechanical polishing is at least not more than 1 μm.

It was confirmed that the identification marks of Examples 1-1, 1-2, and 1-3 had improved visibility for a naked eye as compared with Comparative Example. It was also confirmed that the identification marks which were formed by the methods of Examples 1-2 and 1-3 had further improved visibility for a naked eye as compared with the identification mark which was formed by the method of Example 1-1.

FIG. 6 is an enlarged SEM image showing a portion of a groove of an identification mark which was formed by the method of Example 1-3. As seen from FIG. 6, there was substantially no contaminant on the bottom surface and the lateral surfaces of the groove. Also, there was substantially no unevenness in the internal surface of the groove, and it is appreciated that the surface roughness of the internal surface was very small. Particularly, it can be seen that the bottom surface of the groove was a solidified surface, and it had a striped pattern which was generally perpendicular to the extending direction of the groove. This is probably because a solidified substance was removed by the finishing laser process, and as a result, traces were produced at the bottom surface of the groove due to sequential melting and solidification of silicon carbide single crystal along the traveling direction of the beam spot in the rough laser process, i.e., the scanning direction of the laser beam. Formation of a solidified surface over the internal surface of the groove prevented minute contaminants from remaining on the surface.

It is also seen that edges which defined the groove were also sharp, and the principal surface extending outside the groove was flat. It was confirmed that an identification mark having a desired shape was also formed by the method of Example 1-1. In view of these circumstances, we consider that the identification mark formation methods of Examples 1-1 and 1-3 are more preferred among Examples 1-1, 1-2, and 1-3.

FIGS. 7A and 7B respectively show surface profiles of a cross section perpendicular to, and a cross section parallel to, the extending direction of a groove of an identification mark which was formed by the method of Example 1-3. As seen from these graphs, of the internal surface of the groove, at least the bottom surface had a surface roughness Ra of not more than 1 μm.

FIG. 8 is an enlarged SEM image showing a portion of a groove of an identification mark which was formed by the method of Comparative Example 1-1. As seen from FIG. 8, there were a large number of small solidified substances attached onto the internal surface of the groove so that the internal surface of the groove had an uneven shape. Also, the principal surface extending outside the groove was not flat but had bumps. FIGS. 9A and 9B respectively show a surface profile along a direction perpendicular to the extending direction of a groove of an identification mark formed by the method of Comparative Example 1-1 and a surface profile along the extending direction of that groove. As seen from these graphs, the internal surface of the groove had a surface roughness Ra of not less than several tens of micrometers, so that the internal surface of the groove was not smooth.

From the above results, it was found that an identification mark constituted of a groove which has no contaminant attached onto the internal surface and of which the internal surface is very smooth can be formed by the method of Example 1 in which the rough laser process and the finishing laser process are performed. Employing a mark which is in the form of a groove rather than dots contributes to excellent visibility. It was found that, from the viewpoint of visibility, a kerf width is provided, and the scanning pattern of the laser beam is zigzagged in such a manner that a groove width of not less than about 50 μm is secured, whereby an identification mark with excellent visibility can be formed.

EXAMPLE 2

Hereinafter, an example of formation of an identification mark on a sapphire single crystal substrate with the use of a method for forming an identification mark on a refractory material single crystal substrate according to the second embodiment is described.

A sapphire single crystal substrate with a diameter of 4 inches was provided. The laser light source used for Example 2-1 and Comparative Example 2-1 was a laser manufactured by MIYACHI CORPORATION (wavelength: 532 nm, power: 5 W). The laser light source used for Example 2-2 was a laser manufactured by OMRON Corporation (wavelength: 355 nm, power: 0.4 W). The laser light source used for Example 2-3 was a laser manufactured by Takano Co., Ltd. (wavelength: 266 nm, power: 0.25 W). The laser light source used for Comparative Example 2-2 was a Nd:YAG laser (wavelength: 1064 nm, power: 1.5 W) manufactured by ESI, Inc. These laser light sources had a Q-switch and were used to perform the rough laser process and the finishing laser process under the conditions of Examples 2-1 and 2-2 as shown in Table 4 such that an identification mark of nine characters was formed. In Comparative Examples 2-1 and 2-2, only the rough laser process was performed for formation of an identification mark. In Table 4, the kerf width refers to W2 of FIG. 3. When the kerf width was 0, the principal surface of the substrate was scanned with a laser beam along the extending direction of a groove to be formed. For example, when the width of the groove was about three times the diameter of the laser beam, the principal surface was scanned with the laser beam such that spots in the left column shown in FIG. 3A were drawn, the principal surface was then scanned with the laser beam such that spots in the center column were drawn, and lastly, the principal surface was scanned with the laser beam such that spots in the right column were drawn. In Table 4, the energy density is a relative value which was determined with respect to the energy density of Comparative Example 2-2 which was assumed as 100. In Examples 2-1, 2-2, and 2-3, the energy density of the finishing laser process was made smaller than the energy density of the rough laser process by decreasing the power. The total energy refers to a total energy which was supplied to the substrate by laser beam irradiation for marking a straight line of 1 mm in each of the rough laser process and the finishing laser process. The energy ratio refers to the ratio of the total energy of the finishing laser process to the total energy of the rough laser process.

After the finishing laser process, the mechanical polishing was not performed. The inside of the groove constituting the identification mark was observed with an optical microscope to check whether there was an attached substance, such as a solidified substance, on the bottom surface and the lateral surfaces of the groove. Further, the depth and the width of the groove were measured using an optical length-measuring microscope. The measurement was performed at an arbitrary position in the groove, where the groove width on the substrate surface and the groove depth from the substrate surface were measured. The measurement was carried out at one arbitrary position in each of the grooves of three out of nine characters. Further, the surface roughness Ra of the bottom surface of the groove was measured using the optical interference type surface roughness measuring apparatus HD-2000 manufactured by Veeco Instruments Inc. The measurement was performed on a central portion at an arbitrary position in the groove, along the line direction (the longitudinal direction of the groove), in the length of about 0.2 mm. The measurement was carried out along one arbitrary line in each of the grooves of three out of nine characters. The results are shown in Table 5.

TABLE 4 Example Example Example Comp. Ex. Comp. Ex. 2-1 2-2 2-3 2-1 2-2 Laser Wavelength (nm) 532 355 266 532 1064 Rough Laser Q rate (Hz) 30000 1000 10000 1000 3000 Process Power (%) 100 100 100 80 100 Speed (mm/s) 100 1 1 8 8 Kerf Width 0.15 0 0 0.15 0.15 (mm) Energy 40 60 40 40 100 Density Number of 2 1 7 1 1 Scan Cycles Total 7000 4500 7000 1100 4200 Energy(W) Finish Laser Q rate (Hz) 40000 3000 10000 None None Process Power (%) 80 80 50 Speed (mm/s) 10 3 1 Kerf Width 0 0 0 (mm) Energy 10 20 20 Density Number of 1 1 7 Scan Cycles Total 6000 3000 3500 Energy(W) Energy 85 67 50 Ratio(%)

TABLE 5 Example Example Example Comp. Ex. Comp. Ex. Evaluated Items 2-1 2-2 2-3 2-1 2-2 Cracks Near Groove No No No very Yes small Attached Groove No No No Yes Yes Substance Bottom Inside Wall No No No Yes Yes Groove Surface Groove Before Polish  10  40 10 50 Depth (μm) Groove Before Polish 150 130 90 150-170 Width (μm) After Polish Surface Roughness 0.6-0.8 0.5-0.7 0.76 1-2 3-5 of Groove Bottom Surface Ra (μm)

As seen from Table 5, in Examples 2-1, 2-2, and 2-3, no crack was formed near the groove, and no attached substance was found at the bottom surface or the wall surface of the groove. On the other hand, in Comparative Examples 2-1 and 2-2, cracks were formed near the groove, and attached substances were found at the bottom surface and the wall surface of the groove. This is probably because, in the methods of Examples 2-1, 2-2, and 2-3, solidified substances in the groove were removed by the finishing laser process. It was found from the results of Examples 2-1, 2-2, and 2-3 that attached substances can be entirely removed so long as the energy of the finishing laser process is approximately not less than 50% and not more than 85% of that of the rough laser process. It is understood that, when a margin of about 10% is considered, the energy ratio only needs to be approximately not less than 40% and not more than 95%.

In Examples 2-1, 2-2, and 2-3, the surface roughness Ra of the bottom surface of the groove of the identification mark was in the range of 0.5 μm to 0.8 μm. On the other hand, in Comparative Examples 2-1 and 2-2, the surface roughness Ra of the bottom surface of the groove was in the range of 1.0 μm to 5 μm. It was found from this result that the surface roughness of the internal surface of the groove of the identification mark which was formed according to the methods of Examples 2-1 and 2-2 was improved to, at the maximum, about 1/10 of the surface roughness of the groove which was formed according to the conventional method. It was also found that the surface roughness Ra of the bottom surface of the groove of the identification mark at least in Examples 2-1, 2-2, and 2-3 was not more than 1 λm.

It was confirmed that the identification marks of Examples 2-1, 2-2, and 2-3 had improved visibility for a naked eye as compared with Comparative Examples 2-1 and 2-2.

FIG. 10 is an enlarged optical microscopic image showing a portion of a groove of an identification mark which was formed by the method of Example 2-1. As seen from FIG. 10, no crack was formed near the groove, and there was substantially no contaminant on the bottom surface and the lateral surfaces of the groove. It is also seen that the identification mark can be observed with high visibility although the depth of the groove was 10 μm. FIGS. 11A and 11B show surface profiles of a cross section perpendicular to, and a cross section parallel to, the extending direction of a groove of an identification mark which was formed by the method of Example 2-1. The surface roughness Ra of the bottom surface of the groove was not more than 1 μm.

FIG. 12 is an enlarged optical microscopic image showing a portion of a groove of an identification mark which was formed by the method of Example 2-2. As seen from Table 4, in Example 2-2, the kerf width was 0. This is why scanning with the laser beam was carried out along the extending direction of the groove, and a plurality of scanning traces extending along the groove of the identification mark were also seen in the groove. FIGS. 13A and 13B show surface profiles of a cross section perpendicular to, and a cross section parallel to, the extending direction of a groove of an identification mark which was formed by the method of Example 2-2. As seen from FIG. 13A, in the profile in the direction perpendicular to the groove of the identification mark, there are a plurality of grooves. However, as seen from FIG. 13B, the surface roughness Ra of the bottom surface along the extending direction of the groove is approximately not more than 1 μm.

FIG. 14 is an enlarged optical microscopic image showing a portion of a groove of an identification mark which was formed by the method of Comparative Example 2-1. As seen from FIG. 14, there are cracks in a peripheral region of the groove. The edge of the groove has an irregular shape, so that the edge of the groove is not shaped as designed. Therefore, it is very difficult to discern it as a mark.

From the above results, it was found that an identification mark constituted of a groove which has no contaminant attached onto the internal surface and of which the internal surface is very smooth can be formed by the method of Example 2 in which the rough laser process and the finishing laser process are performed. Employing a mark which is in the form of a groove rather than dots contributes to excellent visibility.

The present invention is suitably applicable to a refractory material single crystal substrate which is used in various uses, including manufacture of a semiconductor device.

While the present invention has been described with respect to preferred embodiments thereof, it will be apparent to those skilled in the art that the disclosed invention may be modified in numerous ways and may assume many embodiments other than those specifically described above. Accordingly, it is intended by the appended claims to cover all modifications of the invention that fall within the true spirit and scope of the invention.

This application is based on Japanese Patent Application No. 2012-154487 filed on Jul. 10, 2012, the entire contents of which are hereby incorporated by reference. 

What is claimed is:
 1. A refractory material single crystal substrate which has an identification mark on a principal surface, the identification mark being constituted of one or more grooves, and the refractory material single crystal substrate being made of a single crystal which is formed by one selected from the group consisting of sapphire, gallium nitride, aluminum nitride, diamond, boron nitride, zinc oxide, gallium oxide, and titanium dioxide, wherein a width of the groove is not less than 50 μm and less than 0.5 mm, and a depth of the groove is not less than 10 μm, and a surface roughness Ra of an internal surface of the groove is not more than 1 μm.
 2. The refractory material single crystal substrate of claim 1, wherein the surface roughness Ra of the principal surface is not less than 0.1 nm and not more than 2.0 nm.
 3. The refractory material single crystal substrate of claim 1, wherein a bottom surface of the groove is a solidified surface.
 4. The refractory material single crystal substrate of claim 3, wherein the bottom surface of the groove has a striped pattern.
 5. The refractory material single crystal substrate of claim 2, wherein a bottom surface of the groove is a solidified surface.
 6. The refractory material single crystal substrate of claim 5, wherein the bottom surface of the groove has a striped pattern. 